Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride
In this study, an adsorbent material made up of a mixture of activated carbon, expanded graphite and lithium chloride, is proposed to evaluate its thermal properties. Ratio effect between mixing components, component particle size, and compaction pressure on porosity and thermal conductivity of comp...
- Autores:
-
Carmona, Mauricio
Pérez, Eduar
Palacio, Mario
- Tipo de recurso:
- Article of journal
- Fecha de publicación:
- 2019
- Institución:
- Universidad Francisco de Paula Santander
- Repositorio:
- Repositorio Digital UFPS
- Idioma:
- eng
- OAI Identifier:
- oai:repositorio.ufps.edu.co:ufps/1729
- Acceso en línea:
- http://repositorio.ufps.edu.co/handle/ufps/1729
https://doi.org/10.1016/j.applthermaleng.2019.01.021
- Palabra clave:
- Thermal conductivity
Porosity
Mixture adsorbent material
Activated carbon
Expanded graphite
Lithium chloride
- Rights
- openAccess
- License
- © 2019 Elsevier Ltd. All rights reserved.
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Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride |
| title |
Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride |
| spellingShingle |
Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride Thermal conductivity Porosity Mixture adsorbent material Activated carbon Expanded graphite Lithium chloride |
| title_short |
Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride |
| title_full |
Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride |
| title_fullStr |
Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride |
| title_full_unstemmed |
Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride |
| title_sort |
Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride |
| dc.creator.fl_str_mv |
Carmona, Mauricio Pérez, Eduar Palacio, Mario |
| dc.contributor.author.none.fl_str_mv |
Carmona, Mauricio Pérez, Eduar Palacio, Mario |
| dc.subject.proposal.eng.fl_str_mv |
Thermal conductivity Porosity Mixture adsorbent material Activated carbon Expanded graphite Lithium chloride |
| topic |
Thermal conductivity Porosity Mixture adsorbent material Activated carbon Expanded graphite Lithium chloride |
| description |
In this study, an adsorbent material made up of a mixture of activated carbon, expanded graphite and lithium chloride, is proposed to evaluate its thermal properties. Ratio effect between mixing components, component particle size, and compaction pressure on porosity and thermal conductivity of composite material was experimentally evaluated. Axial and radial thermal conductivity were evaluated by ASTM C177-13 standard using the hot plate and hot wire method for the respective axial and radial conductivities. Experimental results indicate that the highest porosity reaches 0.78 and is produced with a 70% mixing ratio of activated carbon mass, 10% of LiCl mass, and 20% of expanded graphite mass. With the levels used in experimental design, axial and radial thermal conductivity obtain maximum values of 51.2 W/m K and 11.9 W/m K, respectively. After optimization process based on design of experiments for mixtures, axial and radial conductivity reach their highest values of 76.5 W/m K and 13.8 W/m K, respectively, when mixture is elaborated with a proportion of 30% activated carbon, 40% expanded graphite and 30% Lithium Chloride. This study shows that conductivity results do not vary significantly due to tests temperature. |
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2019 |
| dc.date.issued.none.fl_str_mv |
2019-03-05 |
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2021-12-07T20:45:37Z |
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2021-12-07T20:45:37Z |
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Artículo de revista |
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http://purl.org/coar/resource_type/c_2df8fbb1 |
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http://purl.org/coar/version/c_970fb48d4fbd8a85 |
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http://purl.org/coar/resource_type/c_6501 |
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Text |
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info:eu-repo/semantics/article |
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http://purl.org/redcol/resource_type/ART |
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publishedVersion |
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http://repositorio.ufps.edu.co/handle/ufps/1729 |
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https://doi.org/10.1016/j.applthermaleng.2019.01.021 |
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http://repositorio.ufps.edu.co/handle/ufps/1729 https://doi.org/10.1016/j.applthermaleng.2019.01.021 |
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eng |
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eng |
| dc.relation.ispartof.none.fl_str_mv |
Applied Thermal Engineering |
| dc.relation.citationedition.spa.fl_str_mv |
Vol.150 (2019) |
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463 |
| dc.relation.citationissue.spa.fl_str_mv |
(2019) |
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456 |
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150 |
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Carmona, M., Pérez, E., & Palacio, M. (2019). Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride. Applied Thermal Engineering, 150, 456-463. |
| dc.relation.ispartofjournal.spa.fl_str_mv |
Applied Thermal Engineering |
| dc.rights.eng.fl_str_mv |
© 2019 Elsevier Ltd. All rights reserved. |
| dc.rights.coar.fl_str_mv |
http://purl.org/coar/access_right/c_abf2 |
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info:eu-repo/semantics/openAccess |
| dc.rights.creativecommons.spa.fl_str_mv |
Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0) |
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© 2019 Elsevier Ltd. All rights reserved. Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0) http://purl.org/coar/access_right/c_abf2 |
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openAccess |
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08 páginas |
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application/pdf |
| dc.publisher.spa.fl_str_mv |
Applied Thermal Engineering |
| dc.publisher.place.spa.fl_str_mv |
Reino Unido |
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https://www.sciencedirect.com/science/article/abs/pii/S1359431118355261?via%3Dihub |
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Carmona, Mauricioa5dd98a63f69b923798f638df60881f5600Pérez, Eduar 4f664f5393a466dce30a8fd6974e8f62600Palacio, Mariob6fe00f005dbfc7c4036738515cbafe22021-12-07T20:45:37Z2021-12-07T20:45:37Z2019-03-05http://repositorio.ufps.edu.co/handle/ufps/1729https://doi.org/10.1016/j.applthermaleng.2019.01.021In this study, an adsorbent material made up of a mixture of activated carbon, expanded graphite and lithium chloride, is proposed to evaluate its thermal properties. Ratio effect between mixing components, component particle size, and compaction pressure on porosity and thermal conductivity of composite material was experimentally evaluated. Axial and radial thermal conductivity were evaluated by ASTM C177-13 standard using the hot plate and hot wire method for the respective axial and radial conductivities. Experimental results indicate that the highest porosity reaches 0.78 and is produced with a 70% mixing ratio of activated carbon mass, 10% of LiCl mass, and 20% of expanded graphite mass. With the levels used in experimental design, axial and radial thermal conductivity obtain maximum values of 51.2 W/m K and 11.9 W/m K, respectively. After optimization process based on design of experiments for mixtures, axial and radial conductivity reach their highest values of 76.5 W/m K and 13.8 W/m K, respectively, when mixture is elaborated with a proportion of 30% activated carbon, 40% expanded graphite and 30% Lithium Chloride. This study shows that conductivity results do not vary significantly due to tests temperature.08 páginasapplication/pdfengApplied Thermal EngineeringReino UnidoApplied Thermal EngineeringVol.150 (2019)463(2019)456150Carmona, M., Pérez, E., & Palacio, M. (2019). Experimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride. Applied Thermal Engineering, 150, 456-463.Applied Thermal Engineering© 2019 Elsevier Ltd. All rights reserved.info:eu-repo/semantics/openAccessAtribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0)http://purl.org/coar/access_right/c_abf2https://www.sciencedirect.com/science/article/abs/pii/S1359431118355261?via%3DihubExperimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chlorideArtículo de revistahttp://purl.org/coar/resource_type/c_6501http://purl.org/coar/resource_type/c_2df8fbb1Textinfo:eu-repo/semantics/articlehttp://purl.org/redcol/resource_type/ARTinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/version/c_970fb48d4fbd8a85Thermal conductivityPorosityMixture adsorbent materialActivated carbonExpanded graphiteLithium chlorideH.Z. Hassan, A.A. Mohamad, A review on solar-powered closed physisorption cooling systems, Renew. Sustain. Energy Rev. 16 (5) (2012) 2516–2538.I. Sarbu, C. Sebarchievici, General review of solar-powered closed sorption refrigeration systems, Energy Convers. Manag. 105 (2015) 403–422.H.Z. Hassan, A.A. Mohamad, H.A. Al-Ansary, Development of a continuously operating solar-driven adsorption cooling system: thermodynamic analysis and parametric study, Appl. Therm. Eng. 48 (2012) 332–341.J. Han, K. Cho, K.-H. Lee, H. Kim, Porous graphite matrix for chemical heat pumps, Carbon N. Y. 36 (12) (1998) 1801–1810.X. Zheng, L.W. Wang, R.Z. Wang, T.S. Ge, T.F. Ishugah, Thermal conductivity, pore structure and adsorption performance of compact composite silica gel, Int. J. Heat Mass Transf. 68 (2014) 435–443.J.K. Kiplagat, R.Z. Wang, R.G. Oliveira, T.X. Li, Lithium chloride - expanded graphite composite sorbent for solar powered ice maker, Sol. Energy 84 (9) (2010) 1587–1594.R.G. Oliveira, R.Z. Wang, J.K. Kiplagat, C.Y. Wang, Optimal placement of d resorption systems and for chemisorption air conditioners driven by low generation temperature, Renew. Energy 34 (12) (2009) 2757–2764.S. Mitra, M. Muttakin, K. Thu, B. Baran, Study on the influence of adsorbent particle size and heat exchanger aspect ratio on dynamic adsorption characteristics, Appl. Therm. Eng. J. 133 (2018) 764–773.N. Yu, R.Z. Wang, Z.S. Lu, L.W. Wang, Study on consolidated composite sorbents impregnated with LiCl for thermal energy storage, Int. J. Heat Mass Transf. 84 (2015) 660–670.H. Demir, M. Mobedi, S. Ülkü, Effects of porosity on heat and mass transfer in a granular adsorbent bed, Int. Commun. Heat Mass Transf. 36 (4) (2009) 372–377.K. Fayazmanesh, S. Salari, M. Bahrami, Effective thermal conductivity modeling of consolidated sorption composites containing graphite flakes, Int. J. Heat Mass Transf. 115 (2017) 73–79.A.A. Askalany, S.K. Henninger, M. Ghazy, B.B. Saha, Effect of improving thermal conductivity of the adsorbent on performance of adsorption cooling system, Appl. Therm. Eng. 110 (2017) 695–702.L. Jiang, L.W. Wang, R.Z. Wang, Investigation on thermal conductive consolidated composite CaCl2 for adsorption refrigeration, Int. J. Therm. Sci. 81 (1) (2014) 68–75.L.W. Wang, S.J. Metcalf, R.E. Critoph, R. Thorpe, Z. Tamainot-Telto, Thermal conductivity and permeability of consolidated expanded natural graphite treated with sulphuric acid, Carbon N. Y. 49 (14) (2011) 4812–4819.B. Tian, Z.Q. Jin, L.W. Wang, R.Z. Wang, Permeability and thermal conductivity of compact chemical and physical adsorbents with expanded natural graphite as host matrix, Int. J. Heat Mass Transf. 55 (15–16) (2012) 4453–4459.S. Wu, T.X. Li, T. Yan, Y.J. Dai, R.Z. Wang, High performance form-stable expanded graphite/stearic acid composite phase change material for modular thermal energy storage, Int. J. Heat Mass Transf. 102 (2016) 733–744.X. Xiao, P. Zhang, M. Li, Experimental and numerical study of heat transfer performance of nitrate/expanded graphite composite PCM for solar energy storage, Energy Convers. Manag. 105 (2015) 272–284.F. Cheng, et al., Preparation and analysis of lightweight wall material with expanded graphite (EG)/paraffin composites for solar energy storage, Appl. Therm. Eng. 120 (Jun.) (2017) 107–114.Y. Yang, Y. Pang, Y. Liu, H. Guo, Preparation and thermal properties of polyethylene glycol/expanded graphite as novel form-stable phase change material for indoor energy saving, Mater. Lett. 216 (Apr.) (2018) 220–223.Y. Yuan, H. Bao, Z. Ma, Y. Lu, A.P. Roskilly, “Investigation of equilibrium and dynamic performance of SrCl2-expanded graphite composite in chemisorption refrigeration system,” vol. 147, no. January 2018; 2019, pp. 52–60.H. Heber Green, Studies on the viscosity and conductivity of some aqueous solutions. Part I. Solutions of sucrose, hydrogen chloride, and lithium chloride, J. Chem. Soc. Trans. 1 (1908) 2023–2048.D. Menard, X. Py, N. Mazet, Activated carbon monolith of high thermal conductivity for adsorption processes improvement Part A: adsorption step, Chem. Eng. Process. 44 (2005) 1029–1038.H. Kuwagaki, T. Meguro, J. Tatami, K. Komeya, K. Tamura, An improvement of thermal conduction of activated carbon by adding graphite, J. Mater. Sci. 38 (15) (2003) 3279–3284.ASTM-C177-13, “Standard Test Method for Steady-State Heat Flux Measurements and Thermal Transmission Properties by Means of the Guarded-Hot-Plate,” Annu. B. ASTM Stand., 2014, pp. 1–23.ASTM C136, “Standard Test Method for Sieve Analysis of Fine and Coarse Aggregates,” 2006.R.G. Oliveira, R.Z. Wang, C. Wang, Evaluation of the cooling performance of a consolidated expanded graphite-calcium chloride reactive bed for chemisorption icemaker, Int. J. Refrig. 30 (1) (2007) 103–112.Y. Yang, Y. Pang, Y. Liu, H. Guo, Preparation and thermal properties of polyethylene glycol/expanded graphite as novel form-stable phase change material for indoor energy saving, Mater. Lett. 216 (2018) 220–223.Y. Yuan, H. Bao, Z. Ma, Y. Lu, A.P. Roskilly, Investigation of equilibrium and dynamic performance of SrCl2-expanded graphite composite in chemisorption refrigeration system, Appl. Therm. Eng. 147 (2019,) 52–60 January 2018.N. Yu, R.Z. Wang, Z.S. Lu, L.W. Wang, Development and characterization of silica gel-LiCl composite sorbents for thermal energy storage, Chem. Eng. Sci. 111 (2014) 73–84.I.I. El-sharkawy, A. Pal, T. Miyazaki, B. Baran, A study on consolidated composite adsorbents for cooling application, Appl. Therm. Eng. J. 98 (2016) 1214–1220.L.W. Wang, S.J. Metcalf, R.E. Critoph, Z. Tamainot-telto, R. Thorpe, Two types of natural graphite host matrix for composite activated carbon adsorbents, Appl. Therm. Eng. J. 50 (2013) 1652–1657.K. Fayazmanesh, C. Mccague, M. Bahrami, Consolidated adsorbent containing graphite flakes for heat-driven water sorption cooling systems, Appl. Therm. Eng. J. 123 (2017) 753–760.F.P. Incropera, T.L. Bergman, A.S. Lavine, D.P. DeWitt, Fundamentals of Heat and Mass Transfer, 2011.I.M. Abdulagatov, N.D. Azizov, Densities and apparent molar volumes of concentrated aqueous LiCl solutions at high temperatures and high pressures, Chem. Geol. 230 (1–2) (2006) 22–41.ORIGINALExperimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride.pdfExperimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride.pdfapplication/pdf2939314https://repositorio.ufps.edu.co/bitstream/ufps/1729/1/Experimental%20evaluation%20of%20porosity%2c%20axial%20and%20radial%20thermal%20conductivity%2c%20of%20an%20adsorbent%20material%20composed%20by%20mixture%20of%20activated%20carbon%2c%20expanded%20graphite%20and%20lithium%20chloride.pdf769fe936c9261f39e5a2c9dacdd33a01MD51open accessLICENSElicense.txtlicense.txttext/plain; charset=utf-814828https://repositorio.ufps.edu.co/bitstream/ufps/1729/2/license.txt2f9959eaf5b71fae44bbf9ec84150c7aMD52open accessTEXTExperimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride.pdf.txtExperimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride.pdf.txtExtracted texttext/plain32110https://repositorio.ufps.edu.co/bitstream/ufps/1729/3/Experimental%20evaluation%20of%20porosity%2c%20axial%20and%20radial%20thermal%20conductivity%2c%20of%20an%20adsorbent%20material%20composed%20by%20mixture%20of%20activated%20carbon%2c%20expanded%20graphite%20and%20lithium%20chloride.pdf.txt96a83bfd459b646352c6d551fccc722fMD53open accessTHUMBNAILExperimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by mixture of activated carbon, expanded graphite and lithium chloride.pdf.jpgExperimental evaluation of porosity, axial and radial thermal conductivity, of an adsorbent material composed by 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 incorporada en las Obras Colectivas.

b.	Distribuir copias o fonogramas de las Obras, exhibirlas públicamente, ejecutarlas públicamente y/o ponerlas a disposición pública, incluyéndolas como incorporadas en Obras Colectivas, según corresponda.

c.	Distribuir copias de las Obras Derivadas que se generen, exhibirlas públicamente, ejecutarlas públicamente y/o ponerlas a disposición pública.
Los derechos mencionados anteriormente pueden ser ejercidos en todos los medios y formatos, actualmente conocidos o que se inventen en el futuro. Los derechos antes mencionados incluyen el derecho a realizar dichas modificaciones en la medida que sean técnicamente necesarias para ejercer los derechos en otro medio o formatos, pero de otra manera usted no está autorizado para realizar obras derivadas. Todos los derechos no otorgados expresamente por el Licenciante quedan por este medio reservados, incluyendo pero sin limitarse a aquellos que se mencionan en las secciones 4(d) y 4(e).

4. Restricciones.
La licencia otorgada en la anterior Sección 3 está expresamente sujeta y limitada por las siguientes restricciones:

a.	Usted puede distribuir, exhibir públicamente, ejecutar públicamente, o poner a disposición pública la Obra sólo bajo las condiciones de esta Licencia, y Usted debe incluir una copia de esta licencia o del Identificador Universal de Recursos de la misma con cada copia de la Obra que distribuya, exhiba públicamente, ejecute públicamente o ponga a disposición pública. No es posible ofrecer o imponer ninguna condición sobre la Obra que altere o limite las condiciones de esta Licencia o el ejercicio de los derechos de los destinatarios otorgados en este documento. No es posible sublicenciar la Obra. Usted debe mantener intactos todos los avisos que hagan referencia a esta Licencia y a la cláusula de limitación de garantías. Usted no puede distribuir, exhibir públicamente, ejecutar públicamente, o poner a disposición pública la Obra con alguna medida tecnológica que controle el acceso o la utilización de ella de una forma que sea inconsistente con las condiciones de esta Licencia. Lo anterior se aplica a la Obra incorporada a una Obra Colectiva, pero esto no exige que la Obra Colectiva aparte de la obra misma quede sujeta a las condiciones de esta Licencia. Si Usted crea una Obra Colectiva, previo aviso de cualquier Licenciante debe, en la medida de lo posible, eliminar de la Obra Colectiva cualquier referencia a dicho Licenciante o al Autor Original, según lo solicitado por el Licenciante y conforme lo exige la cláusula 4(c).

b.	Usted no puede ejercer ninguno de los derechos que le han sido otorgados en la Sección 3 precedente de modo que estén principalmente destinados o directamente dirigidos a conseguir un provecho comercial o una compensación monetaria privada. El intercambio de la Obra por otras obras protegidas por derechos de autor, ya sea a través de un sistema para compartir archivos digitales (digital file-sharing) o de cualquier otra manera no será considerado como estar destinado principalmente o dirigido directamente a conseguir un provecho comercial o una compensación monetaria privada, siempre que no se realice un pago mediante una compensación monetaria en relación con el intercambio de obras protegidas por el derecho de autor.

c.	Si usted distribuye, exhibe públicamente, ejecuta públicamente o ejecuta públicamente en forma digital la Obra o cualquier Obra Derivada u Obra Colectiva, Usted debe mantener intacta toda la información de derecho de autor de la Obra y proporcionar, de forma razonable según el medio o manera que Usted esté utilizando: (i) el nombre del Autor Original si está provisto (o seudónimo, si fuere aplicable), y/o (ii) el nombre de la parte o las partes que el Autor Original y/o el Licenciante hubieren designado para la atribución (v.g., un instituto patrocinador, editorial, publicación) en la información de los derechos de autor del Licenciante, términos de servicios o de otras formas razonables; el título de la Obra si está provisto; en la medida de lo razonablemente factible y, si está provisto, el Identificador Uniforme de Recursos (Uniform Resource Identifier) que el Licenciante especifica para ser asociado con la Obra, salvo que tal URI no se refiera a la nota sobre los derechos de autor o a la información sobre el licenciamiento de la Obra; y en el caso de una Obra Derivada, atribuir el crédito identificando el uso de la Obra en la Obra Derivada (v.g., "Traducción Francesa de la Obra del Autor Original," o "Guión Cinematográfico basado en la Obra original del Autor Original"). Tal crédito puede ser implementado de cualquier forma razonable; en el caso, sin embargo, de Obras Derivadas u Obras Colectivas, tal crédito aparecerá, como mínimo, donde aparece el crédito de cualquier otro autor comparable y de una manera, al menos, tan destacada como el crédito de otro autor comparable.

d.	Para evitar toda confusión, el Licenciante aclara que, cuando la obra es una composición musical:

i.	Regalías por interpretación y ejecución bajo licencias generales. El Licenciante se reserva el derecho exclusivo de autorizar la ejecución pública o la ejecución pública digital de la obra y de recolectar, sea individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, SAYCO), las regalías por la ejecución pública o por la ejecución pública digital de la obra (por ejemplo Webcast) licenciada bajo licencias generales, si la interpretación o ejecución de la obra está primordialmente orientada por o dirigida a la obtención de una ventaja comercial o una compensación monetaria privada.

ii.	Regalías por Fonogramas. El Licenciante se reserva el derecho exclusivo de recolectar, individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, los consagrados por la SAYCO), una agencia de derechos musicales o algún agente designado, las regalías por cualquier fonograma que Usted cree a partir de la obra (“versión cover”) y distribuya, en los términos del régimen de derechos de autor, si la creación o distribución de esa versión cover está primordialmente destinada o dirigida a obtener una ventaja comercial o una compensación monetaria privada.

e.	Gestión de Derechos de Autor sobre Interpretaciones y Ejecuciones Digitales (WebCasting). Para evitar toda confusión, el Licenciante aclara que, cuando la obra sea un fonograma, el Licenciante se reserva el derecho exclusivo de autorizar la ejecución pública digital de la obra (por ejemplo, webcast) y de recolectar, individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, ACINPRO), las regalías por la ejecución pública digital de la obra (por ejemplo, webcast), sujeta a las disposiciones aplicables del régimen de Derecho de Autor, si esta ejecución pública digital está primordialmente dirigida a obtener una ventaja comercial o una compensación monetaria privada.

5. Representaciones, Garantías y Limitaciones de Responsabilidad.
A MENOS QUE LAS PARTES LO ACORDARAN DE OTRA FORMA POR ESCRITO, EL LICENCIANTE OFRECE LA OBRA (EN EL ESTADO EN EL QUE SE ENCUENTRA) “TAL CUAL”, SIN BRINDAR GARANTÍAS DE CLASE ALGUNA RESPECTO DE LA OBRA, YA SEA EXPRESA, IMPLÍCITA, LEGAL O CUALQUIERA OTRA, INCLUYENDO, SIN LIMITARSE A ELLAS, GARANTÍAS DE TITULARIDAD, COMERCIABILIDAD, ADAPTABILIDAD O ADECUACIÓN A PROPÓSITO DETERMINADO, AUSENCIA DE INFRACCIÓN, DE AUSENCIA DE DEFECTOS LATENTES O DE OTRO TIPO, O LA PRESENCIA O AUSENCIA DE ERRORES, SEAN O NO DESCUBRIBLES (PUEDAN O NO SER ESTOS DESCUBIERTOS). ALGUNAS JURISDICCIONES NO PERMITEN LA EXCLUSIÓN DE GARANTÍAS IMPLÍCITAS, EN CUYO CASO ESTA EXCLUSIÓN PUEDE NO APLICARSE A USTED.

6. Limitación de responsabilidad.
A MENOS QUE LO EXIJA EXPRESAMENTE LA LEY APLICABLE, EL LICENCIANTE NO SERÁ RESPONSABLE ANTE USTED POR DAÑO ALGUNO, SEA POR RESPONSABILIDAD EXTRACONTRACTUAL, PRECONTRACTUAL O CONTRACTUAL, OBJETIVA O SUBJETIVA, SE TRATE DE DAÑOS MORALES O PATRIMONIALES, DIRECTOS O INDIRECTOS, PREVISTOS O IMPREVISTOS PRODUCIDOS POR EL USO DE ESTA LICENCIA O DE LA OBRA, AUN CUANDO EL LICENCIANTE HAYA SIDO ADVERTIDO DE LA POSIBILIDAD DE DICHOS DAÑOS. ALGUNAS LEYES NO PERMITEN LA EXCLUSIÓN DE CIERTA RESPONSABILIDAD, EN CUYO CASO ESTA EXCLUSIÓN PUEDE NO APLICARSE A USTED.

7. Término.

a.	Esta Licencia y los derechos otorgados en virtud de ella terminarán automáticamente si Usted infringe alguna condición establecida en ella. Sin embargo, los individuos o entidades que han recibido Obras Derivadas o Colectivas de Usted de conformidad con esta Licencia, no verán terminadas sus licencias, siempre que estos individuos o entidades sigan cumpliendo íntegramente las condiciones de estas licencias. Las Secciones 1, 2, 5, 6, 7, y 8 subsistirán a cualquier terminación de esta Licencia.

b.	Sujeta a las condiciones y términos anteriores, la licencia otorgada aquí es perpetua (durante el período de vigencia de los derechos de autor de la obra). No obstante lo anterior, el Licenciante se reserva el derecho a publicar y/o estrenar la Obra bajo condiciones de licencia diferentes o a dejar de distribuirla en los términos de esta Licencia en cualquier momento; en el entendido, sin embargo, que esa elección no servirá para revocar esta licencia o que deba ser otorgada , bajo los términos de esta licencia), y esta licencia continuará en pleno vigor y efecto a menos que sea terminada como se expresa atrás. La Licencia revocada continuará siendo plenamente vigente y efectiva si no se le da término en las condiciones indicadas anteriormente.

8. Varios.

a.	Cada vez que Usted distribuya o ponga a disposición pública la Obra o una Obra Colectiva, el Licenciante ofrecerá al destinatario una licencia en los mismos términos y condiciones que la licencia otorgada a Usted bajo esta Licencia.

b.	Si alguna disposición de esta Licencia resulta invalidada o no exigible, según la legislación vigente, esto no afectará ni la validez ni la aplicabilidad del resto de condiciones de esta Licencia y, sin acción adicional por parte de los sujetos de este acuerdo, aquélla se entenderá reformada lo mínimo necesario para hacer que dicha disposición sea válida y exigible.

c.	Ningún término o disposición de esta Licencia se estimará renunciada y ninguna violación de ella será consentida a menos que esa renuncia o consentimiento sea otorgado por escrito y firmado por la parte que renuncie o consienta.

d.	Esta Licencia refleja el acuerdo pleno entre las partes respecto a la Obra aquí licenciada. No hay arreglos, acuerdos o declaraciones respecto a la Obra que no estén especificados en este documento. El Licenciante no se verá limitado por ninguna disposición adicional que pueda surgir en alguna comunicación emanada de Usted. Esta Licencia no puede ser modificada sin el consentimiento mutuo por escrito del Licenciante y Usted.
 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